Apparatus for simultaneous OTDM demultiplexing, electrical clock recovery and optical clock generation, and optical clock recovery

ABSTRACT

An apparatus for simultaneous OTDM demultiplexing, electrical clock recovery and optical clock generation, and optical clock recovery using a traveling-wave electroabsorption modulator. The apparatus includes a TW-EAM and a PLL coupled thereto. The TW-EAM includes a first, a second, a third, and a fourth. The first port is used for an optical input and the third port is used for optical output. The second port is coupled to an input, and the fourth port is coupled to an output, of the PLL. When the first port receives optical input, the second port produces a photocurrent to be applied to the PLL, and the fourth port receives a recovered clock produced by the PLL, and the third port produces demultiplexed data and an optical clock. Using the same configuration, the apparatus produces a recovered optical clock signal.

PRIORITY CLAIM

Priority is claimed on U.S. patent application Ser. No. 10/800,625,filed Mar. 16, 2004, and provisional U.S. Patent Application Nos.60/458,078, filed Mar. 26, 2003, and 60/459,667, filed Apr. 1, 2003, theentire contents each of which are incorporated herein by reference.

COPYRIGHT RIGHTS

A portion of the material in this patent document is subject tocopyright protection under the copyright laws of the United States andof other countries. The owner of the copyright rights has no objectionto the facsimile reproduction by anyone of the patent document or thepatent disclosure, as it appears in the United States Patent andTrademark Office publicly available file or records, but otherwisereserves all copyright rights whatsoever. The copyright owner does nothereby waive any of its rights to have this patent document maintainedin secrecy, including without limitation its rights pursuant to 37C.F.R. § 1.14.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The invention relates to an apparatus for simultaneous OTDMdemultiplexing, electrical clock recovery and optical clock generation,and to an apparatus for optical clock recovery, using a traveling-waveelectroabsorption modulator.

2. Description of Related Art

Demultiplexing, add/drop, regeneration, clock recovery andsynchronization are the key functions required within an opticaltime-division multiplexing (OTDM) network node. The ability todemultiplex a single channel from a high-speed OTDM data stream andachieve clock recovery to ensure correct synchronization of all datachannels is significant at a network node for further switching anddetection processes. It is desirable to simultaneously performdemultiplexing and clock recovery using a single device to reduce thecost and complexity of the network node. However, the possible problemsof the ambiguity and the crosstalk could occur in the single one devicethat is employed for multiple different purposes at the same time.

Examples of prior attempts to implement simultaneous demultiplexing andclock recovery were made by B. Mikkelsen, G. Raybon, R.-J. Essiambre,“160 Gb/s TDM Transmission Systems,” Paper 6.1.1, pp. 125-128, ECOC2000, and J. Yu, K. Kojima, N. Chand, “Simultaneous Demultiplexing andClock Recovery of 80 Gb/s OTDM Signals Using a Tandem Electro-absorptionModulator,” PDI, pp. 2-3, LEOS 2001.

The ability to generate an optical clock from a high-speed opticaltime-division multiplexed (OTDM) data stream and ensure correctsynchronization is significant in an OTDM network node for all-optical3R (i.e., re-generation). However, usually, it is necessary forrealizing optical clock recovery that an additional photodetector isrequired to detect the data information and an additional pulsegenerator is required to produce the optical clock.

FIG. 15 shows a third example of the related art where discretecomponents for optical clock recovery are used. Data light, which islight having data therein, comes in through a fiber to a clock recoverydevice (CR). The CR has a function of a photodetector and produces anelectrical clock signal. The electrical clock signal is supplied to anexternal intensity modulator (MOD). One example for the MOD is a TW-EAM.On the other hand, a laser diode (LD) radiates a laser beam to the MODwhere the laser beam is modulated by the electrical clock signal. As aresult, the MOD generates an optical clock signal.

FIG. 16 shows a fourth example of the related art where discretecomponents for demultiplexed data recovery are used. Data light signalhaving a bit rate of 40 Gb/s data stream impinges on a photodetector(PD) and an electroabsorption modulator (EAM). In response to the datalight, the PD produces a photocurrent to be supplied to a phase-lockedloop (PLL), which in turn outputs an electrical clock. The electricalclock has a frequency derived by dividing a fundamental frequency of thebit rate of the data stream by, for example, 4, namely 10 GHz that isapplied to the EAM. The EAM produces a bit rate of 10 Gb/s data stream.Also in the fourth example, discrete components of the PD and the EAMare used.

Clock recovery for a signal other than a traveling wave can be explainedby, for example, Japanese Patent Publication Hei 11-38371 disclosed Feb.12, 1999 (Japanese Patent Application Hei 9-189748 filed Jul. 15, 1997).The Publication uses pulsed light as an input signal to be fed into asemiconductor light modulator. The modulator generates a photocurrentthat is applied to a circulator. Regarding pulsed light other than atraveling wave (TW), a circulator is used, but is expensive. On theother hand, a traveling wave does not need an expensive circulator. Inaddition, a traveling wave can be used to produce an electrical clockthat is accurately synchronized with the traveling wave.

Although a TW-EAM is used as a MOD, the TW-EAM is used to only absorband pass incoming light, i.e., is used to modulate the intensity of theincoming light.

Thus, there is a need for one device with respect to a traveling wavethat has the functions of both a photodetector and a modulator, andextracts a clock in incoming data light in addition to absorption andpassing of the data light.

SUMMARY OF THE INVENTION

The invention is a new compact scheme of simultaneous demultiplexing,electrical clock recovery and optical clock generation for OTDM signals.The invention described herein presents a new concept of utilizingindependent electrical frequency division to fulfill simultaneousdemultiplexing, electrical clock recovery and optical clock generationin the same one traveling-wave electroabsorption modulator (TW-EAM)without the ambiguity and the crosstalk problems. The photocurrent ofthe TW-EAM is employed to detect the data information, and thendifferent independent electrical frequency components are simultaneouslyused for recovering the electrical clock through a phase-lock loop(PLL), demultiplexing and optical clock generation, respectively.Accordingly, the TW-EAM works simultaneously as a photodetector, ademultiplexer, and an optical pulse generator. The invention exploitsthe devices multiple functionalities that allow the number of high-speedcomponents within an OTDM network node to be reduced, thereforeincreasing reliability, whilst also substantially reducing costs.

Furthermore, the invention can be extended to two aspects as follows:

(1) Although limited bandwidth of the TW-EAM could restrict the bit rateincrease of the incoming OTDM data stream, an assistant mechanism, suchas extra EAMs or semiconductor optical amplifiers (SOAs), can beintroduced to intentionally produce the desired tones in thephotocurrent of the TW-EAM because the TW-EAM only detects the intensityof the incoming OTDM data. Thus, the scheme can be extended to theapplication of ultra-high speed OTDM system.

(2) More functionalities in a single TW-EAM could be achievedsimultaneously when the dimensions of the TW-EAM such asbidirectionality and states of polarization are further employed.

Moreover, the invention is another new scheme to achieve optical clockrecovery that the photocurrent in a traveling-wave electroabsorptionmodulator (TW-EAM) is used to detect the data information and then therecovered electrical clock from a phase-lock loop (PLL) is employed tomodulate the TW-EAM.

The invention exploits the low-cost implementation of optical clockrecovery by using a TW-EAM with two electrical ports and two opticalports wherein the TW-EAM can work as a photodiode and pulse generatorsimultaneously. On one hand, the photocurrent of the TW-EAM detects thedata information that is then employed for recovering the electricalclock through the PLL. On the other hand, the electrical recovery clockis used to modulate the TW-EAM and generate an optical clock at anotherwavelength. Accordingly, the TW-EAM works as a photodiode and a pulsegenerator simultaneously so that the number of the required componentsfor optical clock recovery can be reduced, thereby substantiallyreducing the cost.

Further aspects of the invention will be brought out in the followingportions of the specification, wherein the detailed description is forthe purpose of fully disclosing preferred embodiments of the inventionwithout placing limitations thereon.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a schematic diagram for illustrating a general function of theinvention.

FIG. 2 is a schematic diagram for illustrating a basic configuration andprinciple of operation of one embodiment of the present invention.

FIG. 3 is an RF spectrum of a photocurrent from TW-EAM under 40 Gb/sdata input.

FIG. 4 shows a locking range under 40 Gb/s input.

FIG. 5 shows bit-error-rate results with transmitter clock and recoveredclock.

FIG. 6A shows Bsingle side band (SSB) noise spectra for transmitterclock, electrical recovered clock and generated optical clock.

FIG. 6B shows a corresponding radio frequency (RF) spectrum at 1 kHzRBW.(Resolution Bandwidth).

FIG. 7 shows a modified scheme for an application of ultra-high speedOTDM signals.

FIG. 8 shows bit-error-rate results with transmitter clock and recoveredclock.

FIG. 9A shows SSB noise spectra for transmitter clock, electricalrecovered clock and generated optical clock.

FIG. 9B shows a corresponding RF spectrum at 1 kHz resolution bandwidth(RBW).

FIG. 10 is a schematic diagram for network architecture of oneembodiment of the invention.

FIG. 11 is a schematic diagram for one preferred embodiment of theinvention usin. g a four-port TW-EAM.

FIG. 12 shows an RF spectrum of a photocurrent from the TW-EAM under 40Gb/s data input.

FIG. 13 shows a locking range under 40 Gb/s input.

FIG. 14 shows a 40 GHz recovery electrical clock for 40 Gb/s OTDM datainput.

FIG. 15 shows a third example of the related art where discretecomponents for optical clock recovery are used.

FIG. 16 shows a fourth example of the related art where discretecomponents for demultiplexed data recovery are used.

DETAILED DESCRIPTION OF THE INVENTION

The invention presents a new scheme for simultaneous OTDM signaldemultiplexing, electrical clock recovery and optical clock generationusing single one TW-EAM in order to reduce the cost and complexity ofthe network node. Except that the TW-EAM works as a compactdemultiplexing receiver, another possible application is to convert highbit rate OTDM data to low bit rate.

FIG. 1 is a schematic diagram that illustrates a general function of theinvention. The ability to convert all channels of a high-speed OTDM datastream to a low-speed data stream with correct synchronization issignificant at a network node for future processing such as from corenetwork to access network. Thus, the relatively low-speed and low-costequipments can be used for switching and detection purposes even when anultra-high speed OTDM data stream enters the node. Depending on thetypes of the 3R regenerators (all-optical or optoelectric), eithergenerated optical clock or recovered electrical clock can be used.

Referring now to FIG. 2, the basic configuration and principle ofoperation of one embodiment of the present invention is illustrated. Inthe embodiment shown, a four-port TW-EAM is used. Port 1 and Port 3 areused for the optical input and output; Port 2 and Port 4 are used toextract the clock information from the photocurrent of the TW-EAM forthe PLL operation and modulate the TW-EAM with the recovered electricalclock, respectively.

When a 40 Gb/s OTDM data stream with the wavelength λ₁ enters theTW-EAM, its information that is imposed as the intensity modulation isdetected by the photocurrent of the TW-EAM, which is shown in FIG. 3.The 40 GHz tone in the photocurrent shown in FIG. 3 represents theinformation of the fundamental frequency of intensity modulation of theincoming optical 40 Gb/s data, including the phase. Then, it isextracted from the photocurrent by a 40 GHz RF band-pass filter (BPF) ina phase-lock loop (PLL) for 10 GHz electrical clock recovery.Afterwards, the electrical recovered clock is applied to drive theTW-EAM for OTDM demultiplexing after its phase adjustment and its RFpower amplification. Simultaneously, 10 GHz optical clock withwavelength λ₂ is generated during the demultiplexing process when a CWlight beam with λ₂ goes through the TW-EAM. It is desirable that the 10GHz optical clock can be used to do 3R regeneration or whatever else ata lower bit rate for future processing.

Note that it is important that independent electrical frequency divisionis employed to achieve three co-existing functions in an TW-EAM withoutthe crosstalk and the ambiguity, i.e., when the 10 GHz recoveredelectrical clock was used to modulate the TW-EAM for demultiplexing andoptical clock generation, different frequency component of 40 GHz tonefrom the photocurrent was extracted for clock recovery by the PLL. Thus,although a mixed signal of 40 GHz and 10 GHz electrical signals entersthe PLL, the 10 GHz clock can be easily removed by the narrowband 40 GHzBPF in the PLL. So, the TW-EAM works simultaneously as a photodetector,a demultiplexer, and an optical pulse generator.

The configuration shown in FIG. 2 and principle of operation describedin connection with FIG. 2 represents the preferred embodiment of theinvention. The locking range of the configuration was measured under 40Gb/s data input, which is shown in FIG. 4. About 200 kHz locking rangeat 0 dBm optical input power and about 700 kHz at 5 dBm optical inputpower were obtained, respectively.

FIG. 5 shows the bit-error-rate (BER) curves and the eye diagrams. BERcomparison is done by switching the 10 GHz electrical clock supplied tothe TW-EAM and the BER tester from the transmitter clock (back-to-back)to the recovered electrical clock.

FIG. 6A shows single side band (SSB) noise spectra for transmitterclock, recovered electrical clock and generated optical clock. FIG. 6Bshows a corresponding RF spectrum at 1 kHz resolution bandwidth (RBW).As shown in FIGS. 6A and 6B, total root mean square (RMS) jitter for thetransmitter clock is 0.02731 rad, the electrical clock recovered fromthe PLL is 0.02757 rad and the generated optical clock is 0.02758 rad,respectively. It is obvious that the RMS jitter mainly comes from thetransmitter clock. The inset waveforms in FIG. 6A show the 10 GHzrecovered electrical clock and generated optical clock. The pulse widthof the optical clock is about 14-ps.

The limited bandwidth of the TW-EAM could restrict the application ofthe scheme to ultra-high speed OTDM system. However, when an assistantmechanism is introduced to intentionally produce the desired tones inthe photocurrent, such as 40 GHz or 10 GHz, the scheme can be extendedto ultra-high speed OTDM application. A possible assistant mechanism isto introduce another EAM that is used for demultiplexing the ultra-highspeed OTDM signals to relatively low-speed OTDM signals that can behandled by the TW-EAM. For example, as shown in FIG. 7, an extra EAM(EAM 2) is added to demultiplex 160 Gb/s OTDM signals to 40 Gb/s andthen the demultiplexed 40 Gb/s OTDM signals enter the TW-EAM (EAM 1).The dominated 40 GHz tone in the photocurrent of the TW-EAM is used bythe PLL to recover 10 GHz electrical clock. The 10 GHz electricalrecovered clock and its fourth times 40 GHz electrical clock are used todemultiplex 40 Gb/s and 160 Gb/s OTDM signals in the EAM 1 and EAM 2,respectively. When an extra CW light beam with wavelength λ₂ and with λ₃enters the EAM 1 and EAM 2, respectively, both 10 GHz and 40 GHz opticalclocks can be generated at the same time, which can be used to do 3Rregeneration at a lower bit rate. Furthermore, in usingcounter-propagation scheme, the clock wavelength can even be the same asthe OTDM data wavelength.

FIG. 8 shows the BER results of simultaneous demultiplexing and clockrecovery for 160 Gb/s OTDM signals. Error free operation and as low as0.5 dB power penalty were obtained, respectively.

FIG. 9A shows SSB noise spectra for transmitter clock, electricalrecovered clock and generated optical clock. FIG. 9B shows acorresponding RF spectrum at 1 kHz RBW. As shown in FIGS. 9A and 9B,total RMS jitter for the transmitter clock is 0.02693 rad, theelectrical clock recovered from the PLL is 0.02697 rad and the generatedoptical clock is 0.02715 rad, respectively. Also, it is obvious that theRMS jitter mainly comes from the transmitter clock. The inset waveformsin FIG. 9A show the 10 GHz recovered electrical clock and generatedoptical clock.

The present invention is advantageous since the TW-EAM can worksimultaneously as a photodetector, a demultiplexer, and an optical pulsegenerator. Photocurrent of TW-EAM and independent frequency divisionmake it feasible to achieve three co-existing functions in a TW-EAMwithout the crosstalk and the ambiguity.

Furthermore, the scheme can be extended to two aspects: (1) Althoughlimited bandwidth of the TW-EAM restricts the bit rate increase of theincoming OTDM data stream, an assistant mechanism can be introduced tointentionally produce the desired tones in the photocurrent of theTW-EAM because it only reflects the intensity of the incoming OTDM data.Thus, the scheme can be extended to the application of ultra-high speedOTDM system. (2) More functionalities in a single TW-EAM can be achievedsimultaneously when the dimensions of the TW-EAM such asbidirectionality and states of polarization are employed.

The invention presents another new scheme for optical clock recovery bycombining a TW-EAM and a PLL. The generated optical clock has manyapplications, such as all-optical 3R regeneration. FIG. 10 shows thenetwork architecture of one embodiment of the invention for all-optical3R regeneration.

FIG. 11 is a schematic diagram for one preferred embodiment of theinvention using a four-port TW-EAM, and shows a configuration andprinciple thereof. In this embodiment, Port 1 and Port 3 are used forthe optical input and output; Port 2 and Port 4 are used to extract thedata information from the photocurrent of the TW-EAM for the PLLoperation and to modulate the TW-EAM with the recovered electricalclock, respectively.

When a 40 Gb/s OTDM data stream with the wavelength λ₁ enters theTW-EAM, its information that is imposed as the intensity modulation isdetected by the photocurrent of the TW-EAM. An RF spectrum of thephotocurrent is shown in FIG. 12. The 40 GHz tone in the spectrum forthe photocurrent shown in FIG. 12 represents the information of thefundamental frequency of intensity modulation of the incoming optical 40Gb/s data, including the phase. Then, it is extracted from thephotocurrent by a 40 GHz RF band-pass filter in a phase-lock loop (PLL)for 40 GHz electrical clock recovery. Afterwards, the 40 GHz electricalrecovery clock is applied to modulate the TW-EAM after its phaseadjustment and its RF power amplification. When a CW light beam withwavelength λ₂ goes through the TW-EAM, a 40 GHz optical clock with λ₂ isgenerated.

The locking range of the configuration shown in FIG. 11 was measured fora 40 Gb/s data input, and the results are shown in FIG. 13. About 200kHz locking range at 0 dBm optical input power and about 700 kHz at 5dBm optical input power were obtained, respectively.

FIG. 14 shows a 40 GHz recovery electrical clock when 40 Gb/s OTDM dataenters the configuration.

The invention is advantageous since the TW-EAM can work simultaneouslyas a photodetector and an optical pulse generator: (1) the photocurrentof the TW-EAM detects the data information which is then employed forrecovering the electrical clock through the PLL; (2) the recoveredelectrical clock is fed to modulate the TW-EAM and generate an opticalclock with another wavelength. Therefore, it is possible in the futureto reduce the number of the required components for lightwave functionstherefore substantially reducing the cost.

While preferred embodiments of the invention have been described andillustrated above, it should be understood that these are exemplary ofthe invention and are not to be considered as limiting. Additions,omissions, substitutions, and other modifications can be made withoutdeparting from the spirit or scope of the present invention.Accordingly, the invention is not to be considered as being limited bythe foregoing description, and is only limited by the scope of theappended claims.

1-8. (canceled) 9: An apparatus for optical clock recovery, comprising:a traveling-wave electroabsorption modulator; and a phase-locked loop(PLL) coupled to said traveling-wave electroabsorption modulator,wherein photocurrent of the traveling-wave electroabsorption modulatoris used to detect data and recover an electrical clock through the PLL,wherein the recovered electrical clock is used to modulate thetraveling-wave electroabsorption modulator and generate an optical clockat a different wavelength, and wherein said traveling-waveelectroabsorption modulator operates simultaneously as a photodiode anda pulse generator. 10: An apparatus as recited in claim 9, wherein saidtraveling-wave electroabsorption modulator includes a first port coupledto the PLL and configured to output a photocurrent, and a second portcoupled to the PLL, wherein the photocurrent from the first port of saidtraveling-wave electroabsorption modulator provides a tone to said PLL,and wherein said PLL provides a recovered electrical clock signal to asecond port of said traveling-wave electroabsorption modulator. 11: Anapparatus as recited in claim 9, wherein said optical clock is used forall optical 3R regeneration. 12: An apparatus for optical clockrecovery, comprising: a traveling-wave electroabsorption modulator; anda phase-locked loop coupled to said traveling-wave electroabsorptionmodulator, wherein photocurrent of the traveling-wave electroabsorptionmodulator is used to detect data and recover an electrical clock throughthe phase locked loop, wherein the recovered electrical clock is used tomodulate the traveling-wave electroabsorption modulator and generate anoptical clock at a different wavelength, wherein the photocurrent from afirst port of said traveling wave electroabsorption modulator provides atone to said phase-locked loop, wherein said phase locked loop providesa recovered electrical clock signal to a second port of saidtraveling-wave electroabsorption modulator, and wherein saidtraveling-wave electroabsorption modulator operates simultaneously as aphotodiode and a pulse generator. 13: An apparatus as recited in claim12, wherein said optical clock is used for all optical 3R regeneration.14-23. (canceled)